Energy & Power · Study deck

Low-Power Design: Leakage and Body Bias

A transistor can leak even when it is off.

Battery Bruno is your guide for this deck.

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Battery Bruno, the module guide, in a scene from this chapter.
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After studying this chapter

Learning objectives

You will be able to:

  • Test subthreshold slope and the leakage-speed trade with a concrete scenario and pass criteria.
  • Validate concrete nanowatt adc and input amplifier with a concrete scenario and pass criteria.
  • test subthreshold slope and the leakage-speed trade with a concrete scenario and pass criteria
  • validate concrete nanowatt adc and input amplifier with a concrete scenario and pass criteria
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Major section

Subthreshold Slope and the Leakage-Speed Trade

A MOSFET does not become an ideal open switch when $V_{GS}$ crosses below threshold.

  • where $U_T=kT/q$ is thermal voltage and $n\ge1$ is the subthreshold slope factor.
  • Taking a base-10 logarithm gives.
  • The subthreshold swing—the gate-voltage change needed for one decade of drain-current change—is therefore.

Why it matters

Raising $V_T$ shifts the exponential curve and reduces off-current roughly by a decade per $S$ millivolts, but it also reduces overdrive $V_{GS}-V_T$ in the on state.

Log drain current versus gate voltage for a low-V~T~ and a high-V~T~ device: parallel subthreshold slopes, off-currents decades apart, on-currents close together.
Log drain current versus gate voltage for a low-V~T~ and a high-V~T~ device: parallel subthreshold slopes, off-currents decades apart, on-currents close together.
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Major section

Subthreshold Slope and the Leakage-Speed Trade (continued)

At 300 K, $kT/q\approx25.85$ mV, so the ideal $n=1$ limit is $S\approx59.6$ mV/decade.

  • The often quoted “60 mV per decade” is thus not simply $kT/q$; it includes $\ln10$, and practical devices have $n>1$.
  • Higher temperature makes the slope worse.
  • Lower drive current increases delay.
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Major section

FD-SOI Forward and Reverse Body Bias

The body is depleted, and the isolated back gate can electrostatically shift threshold with less junction leakage than a conventional bulk body connection.

  • Flipped-well layouts can make wider back-bias choices available for low-threshold devices, while regular-threshold arrangements use different well and nominal-bias connections.

Why it matters

For an NMOS, forward body bias moves the body positive relative to the source and reduces $V_T$; reverse body bias moves it negative and raises $V_T$.

FD-SOI body bias: the well under the buried oxide acts as a back gate; forward bias lowers the threshold for speed, reverse bias raises it for decades less leakage.
FD-SOI body bias: the well under the buried oxide acts as a back gate; forward bias lowers the threshold for speed, reverse bias raises it for decades less leakage.
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Major section

FD-SOI Forward and Reverse Body Bias (continued)

The exact safe rails—sometimes spanning several volts in a characterized FD-SOI process—are process rules, not portable firmware constants.

  • for NMOS under the sign convention above, where $\eta$ is the process-dependent body factor.
  • Substituting the shifted $V_T$ into the weak-inversion equation shows why a modest reverse bias can reduce $I_{OFF}$ exponentially.
  • That asymmetry is what an adaptive bias schedule exploits.
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Major section

FD-SOI Forward and Reverse Body Bias (continued)

Substituting it into an on-current model such as $I_{ON}\propto(V_{GS}-V_T)^\alpha$ shows the simultaneous loss of drive.

  • An adaptive policy can therefore apply forward bias for a deadline-bound active burst and reverse bias during a long retained sleep.
  • It must budget bias-generator current, rail-settling time, reliability limits, temperature, and the energy of changing modes.
  • Firmware should select only documented operating points and wait for the silicon's ready indication; transistor cross-sections and well voltages belong to the chip's process documentation.
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Major section

Low-Frequency Front-End Noise

A sample-and-hold and ADC then create discrete-time codes for digital processing.

  • Below that line the converter contributes kT/C and quantization terms of its own, and the closing card states the rule the whole budget rests on: everything added upstream is baked into the samples.
Anatomy of an analog-digital interface: sensor, low-noise amplifier, anti-alias filter, sample-and-hold, SAR ADC with reference, and the digital word — each stage annotated with its noise contribution and energy cost.
Anatomy of an analog-digital interface: sensor, low-noise amplifier, anti-alias filter, sample-and-hold, SAR ADC with reference, and the digital word — each stage annotated with its noise contribution and energy cost.
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Major section

Low-Frequency Front-End Noise (continued)

The corner $f_c$ is where $K_f/f_c^\alpha=S_{white}$.

  • Below $f_c$, integrating flicker noise over $f_L$ to $f_H$ for $\alpha=1$ gives.
  • If the signal spectrum sits below $f_c$, the amplifier's offset, drift, and flicker noise can swamp it before the ADC sees a useful separation.
  • The review must therefore compare input-referred signal range, offset after calibration, integrated noise across the actual bandwidth, and ADC LSB size at the amplifier output.
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Major section

Chopper Amplifier Signal Path

Chopper stabilization separates a low-frequency input from the amplifier's own low-frequency error by multiplying twice with a square wave $m(t)\in\{-1,+1\}$.

  • The amplifier processes that modulated signal.
  • Its offset and internal $1/f$ noise are added after the first mixer and therefore remain near baseband at this point.
  • Chopping is not magic.

Numbers to remember

50%An ideal 50% square wave has odd-harmonic coefficients proportional to $1/(2k+1)$
The chopper path — mixer, amplifier, mixer, low-pass filter — and the spectrum at three points: the signal rides out to odd harmonics of f_chop and back, while offset and 1/f noise make only the outward trip.
The chopper path — mixer, amplifier, mixer, low-pass filter — and the spectrum at three points: the signal rides out to odd harmonics of f_chop and back, while offset and 1/f noise make only the outward trip.
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Major section

Chopper Amplifier Signal Path (continued)

The amplifier offset and low-frequency noise are multiplied only once, so they move to $f_{chop}$ and its odd harmonics.

  • A low-pass filter passes the recovered sensor band and rejects the translated error and switching artifacts.
  • An ideal 50% square wave has odd-harmonic coefficients proportional to $1/(2k+1)$, so the first modulation produces replicas around $f_{chop},3f_{chop},5f_{chop},\ldots$.
  • The small gray chop artifacts at even harmonics are the residue real switches add.
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Major section

Concrete Nanowatt ADC and Input Amplifier

A 1 ksample/s converter has a 1 ms sample period.

  • If off-state power were negligible, the equivalent active power during the 5 $\mu$s window would be $1\ \text{nW}/0.005=200$ nW.
  • The paired input amplifier provides a separate lesson.
  • The reported input-referred noise of 26 $\mu$V rms becomes about.

Why it matters

The servo corner must sit below the wanted band; otherwise it will cancel part of the signal.

A nanowatt front end as two contracts: a SAR ADC active for 5 µs of every 1 ms sample period, and an AC-coupled 32 dB amplifier whose slow DC servo returns the output baseline to the input.
A nanowatt front end as two contracts: a SAR ADC active for 5 µs of every 1 ms sample period, and an AC-coupled 32 dB amplifier whose slow DC servo returns the output baseline to the input.
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Major section

Concrete Nanowatt ADC and Input Amplifier (continued)

A real ledger must keep clock generation, reference settling, leakage, tracking, and output logic in the appropriate window rather than attributing everything to the comparator search.

  • AC coupling blocks sensor and electrode DC offsets from consuming output range, while a slow DC-servo loop feeds back the residual output baseline so the signal path remains centered.
  • A stated 370 Hz bandwidth then bounds the upper useful signal content and informs anti-alias filtering before 1 ksample/s conversion.
  • The result is compelling precisely because it is a complete front-end timing and noise contract, not because “nanowatt” appears on one block.
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Deck summary

Key takeaways

A MOSFET does not become an ideal open switch when $V_{GS}$ crosses below threshold.

  • At 300 K, $kT/q\approx25.85$ mV, so the ideal $n=1$ limit is $S\approx59.6$ mV/decade.
  • The body is depleted, and the isolated back gate can electrostatically shift threshold with less junction leakage than a conventional bulk body connection.
  • The exact safe rails—sometimes spanning several volts in a characterized FD-SOI process—are process rules, not portable firmware constants.
  • Substituting it into an on-current model such as $I_{ON}\propto(V_{GS}-V_T)^\alpha$ shows the simultaneous loss of drive.
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Retrieval practice

Recall check

Battery Bruno says: answer from memory, then check your reasoning.

Q1A chip designer raises transistor threshold to reduce standby leakage. Which competing effect should be expected?

AZero off-current once the gate is below threshold
BA temperature-independent standby behavior
CLess on-state drive and increased delay
DGreater speed with the same control voltage
Show answer

Answer: C The chapter links reduced leakage to lower overdrive and slower switching.

Q2An FD-SOI design applies reverse body bias to save standby energy. What trade-off does the table predict?

ASafe bias rails copied unchanged across processes
BHigher threshold magnitude and lower drive speed
CLower threshold magnitude with reduced leakage
DHigher speed without an off-current change
Show answer

Answer: B Reverse bias reduces off-current while reducing on-current and speed.

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Print reference

Answers

Answer key.

  1. C · The chapter links reduced leakage to lower overdrive and slower switching.
  2. B · Reverse bias reduces off-current while reducing on-current and speed.
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